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Short-range magnetic behavior in manganites La0.93K0.07Mn1- x Cu x O3 (0.0 ⩽ x ⩽ 0.09) above the Curie temperature
Journal of Physics D: Applied Physics ( IF 3.1 ) Pub Date : 2021-02-12 , DOI: 10.1088/1361-6463/abde6b
Fatma Khammassi 1 , Jose F Lpez 2 , Wajdi Chrif 1 , Aminta Mendoza 2 , Senentxu Lanceros-Mendez 3, 4 , Mohamed Dammak 1 , Daniel Salazar 3
Affiliation  

Manganites La0.93K0.07Mn1−x Cu x O3 $(0.0\,\leqslant\,x\,\leqslant\,0.09),$ prepared by the solid state reaction method at high temperature, were studied structurally and magnetically. The unit cell parameters, as well as bond length ${{\text{d}}_{({\text{Mn,Cu)-O}}}}{\text{ }}\left({{{\unicode{x00C5}}}} \right)$ and the bond angle ${\theta _{({\text{Mn,Cu)-}}{{\text{O}}_{\text{1}}}{\text{-Mn}}}}$, were determined from the Rietveld refinement of the x-ray diffraction patterns. The Fourier-transform infrared spectroscopy analysis shows that Cu2+ substitution induces variations in the vibration modes of the MnO6 octahedra. Magnetization vs. temperature ${\text{M}}\left( T \right)$ at low magnetic field $H = 0.01{ }T$ were performed in the range $5 < T < 300{{\,K}}$ under field coolingand zero field cooling conditions. All the samples exhibited a second-order paramagnetic–ferromagnetic (FM) transition at Curie temperature, ${T_{\text{C}}}$, in the range between 199 and 285 K. The inverse susceptibility, ${\chi ^{ - 1}}\left( T \right){ }$ exhibits a linear Curie-Weiss (C-W) behavior for $T > T_{{\text{CW}}}^{\text{*}}$, while for ${T_{\text{C}}} < T < T_{{\text{CW}}}^{\text{*}}$, it shows a deviation from the linear behavior predicted by the Heisenberg model. The mentioned deviation of ${\chi ^{ - 1}}\left( T \right)$ means that a short ferromagnetic state formation is present even for $T > {T_{\text{C}}}$, which were characterized by the experimental effective magnetic moment, $\mu _{{\text{eff}}}^{{\text{exp}}}.$ A null spontaneous magnetization, ${{\text{m}}_{\text{S}}},$ above ${T_{\text{C}}}$ was evaluated for all samples by using the Kouvel-Fisher method. This work evaluates the short-range FM clusters by means of an extension of the C-W approach to the ${T_{\text{C}}} < T < T_{{\text{CW}}}^{\text{*}}$ region, i.e., ${ }\mu _{{\text{eff}}}^{{\text{exp}}}\left( T \right) = 2.3\sqrt {{\text{C}}\left( T \right)} { }{\mu _{\text{B}}}$. Finally, the critical coefficient values, $\beta $ and $\gamma $, showed that the 3D Heisenberg model fits adequately the $x = 0.0{ }$ and $x = 0.03$ samples, while the 3D Ising model fits the $x = 0.09$ sample.



中文翻译:

在锰氧化物短程磁性行为的La 0.93 ķ 0.071- X的Cu X ø 3(0.0⩽ X高于居里温度⩽0.09)

在结构和磁性上研究了通过高温固态反应法制备的锰La 0.93 K 0.07 Mn 1- x Cu x O 3。单位晶胞参数,以及键长和键角,是根据X射线衍射图的Rietveld精修确定的。傅立叶变换红外光谱分析表明,Cu 2+取代引起MnO 6八面体振动模式的变化。在低磁场下进行磁化强度与温度的关系 $(0.0 \,\ leqslant \,x \,\ leqslant \,0.09),$$ {{\ text {d}} _ {{{text {Mn,Cu)-O}}}} {\ text {}} \ left({{{\ unicode {x00C5}}}}} \ right)$$ {\ theta _ {({\ text {Mn,Cu)-}} {{\ text {O}} _ {\ text {1}}} {\ text {-Mn}}}} $$ {\ text {M}} \ left(T \ right)$$ H = 0.01 {} T $$ 5 <T <300 {{\,K}} $在野外冷却和零野外冷却条件下。所有的样品在居里温度显示出二阶顺磁性铁磁(FM)过渡,$ {T _ {\ text {C}}} $在逆易感性199和K. 285之间的范围内,$ {\ chi ^ {-1}} \ left(T \ right){} $显示出用于线性居里-外斯(CW)的行为$ T> T _ {{\ text {CW}}} ^ {\ text {*}} $,而$ {T _ {\ text {C}}} <T <T _ {{\ text {CW}}} ^ {\ text {*}} $,它示出了与海森堡模型预测的线性行为的偏差。所提到的偏差$ {\ chi ^ {-1}} \ left(T \ right)$的装置,一个短铁磁态的形成是本即使对$ T> {T _ {\ text {C}}} $,将其特征在于所述的实验有效磁矩,$ \ mu _ {{\ text {eff}}} ^ {{\ text {exp}}}。$空自发磁化,$ {{\ text {m}} _ {\ text {S}}},$上述$ {T _ {\ text {C}}} $使用Kouvel-Fisher方法对所有样品进行了评估。这项工作通过将CW方法扩展到该$ {T _ {\ text {C}}} <T <T _ {{\ text {CW}}} ^ {\ text {*}} $区域(即)来评估短程FM群集$ {} \ mu _ {{\ text {eff}}} ^ {{\ text {exp}}} \ left(T \ right)= 2.3 \ sqrt {{\ text {C}} \ left(T \ right )} {} {\ mu _ {\ text {B}}} $。最后,临界系数值$ \ beta $$ \伽马$表示3D Heisenberg模型足够适合$ x = 0.0 {} $$ x = 0.03 $样本,而3D Ising模型适合$ x = 0.09 $样本。

更新日期:2021-02-12
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